External electron pair production in high-energy collisions

1996 ◽  
Vol 109 (11) ◽  
pp. 1517-1528 ◽  
Author(s):  
M. El-Nadi ◽  
S. Kamel ◽  
A. Hussein ◽  
Z. Abou-Moussa ◽  
E. A. Shaat ◽  
...  
Keyword(s):  
Pair Production ◽  
Electron Pair ◽  
High Energy ◽  
High Energy Collisions

scholarly journals Electron Pair Production at High Energy in a Silicon Single Crystal

1960 ◽  
Vol 4 (3) ◽  
pp. 134-135 ◽  
Author(s):  
G. Bologna ◽  
G. Diambrini ◽  
G. P. Murtas
Keyword(s):  
Single Crystal ◽  
Pair Production ◽  
Electron Pair ◽  
High Energy ◽  
Silicon Single Crystal

Direct Electron Pair Production by High-Energy Muons

1974 ◽  
Vol 32 (25) ◽  
pp. 1460-1463 ◽  
Author(s):  
P. L. Jain ◽  
M. Kazuno ◽  
B. Girard
Keyword(s):  
Pair Production ◽  
Electron Pair ◽  
High Energy

High-energy electron pair production on oxygen

1991 ◽  
Vol 30 (9) ◽  
pp. 1235-1248 ◽  
Author(s):  
George L. Strobel1 ◽  
Robert A. Koss
Keyword(s):  
Pair Production ◽  
Electron Pair ◽  
High Energy ◽  
Energy Electron ◽  
High Energy Electron

scholarly journals High-energy γ -photon polarization in nonlinear Breit-Wheeler pair production and γ polarimetry

2020 ◽  
Vol 2 (3) ◽  
Author(s):  
Feng Wan ◽  
Yu Wang ◽  
Ren-Tong Guo ◽  
Yue-Yue Chen ◽  
Rashid Shaisultanov ◽  
...  
Keyword(s):  
Pair Production ◽  
High Energy ◽  
Photon Polarization

scholarly journals Strangeness Suppression and Color Deconfinement

2018 ◽  
Vol 171 ◽  
pp. 02005
Author(s):  
Helmut Satz
Keyword(s):  
Initial Temperature ◽  
Strange Particle ◽  
High Energy ◽  
Universal Function ◽  
Ideal Gas ◽  
Entropy Density ◽  
Suppression Factor ◽  
Thermal Medium ◽  
High Energy Collisions ◽  
Hadronic Resonances

The relative multiplicities for hadron production in different high energy collisions are in general well described by an ideal gas of all hadronic resonances, except that under certain conditions, strange particle rates are systematically reduced. We show that the suppression factor γs, accounting for reduced strange particle rates in pp, pA and AA collisions at different collision energies, becomes a universal function when expressed in terms of the initial entropy density s0 or the initial temperature T of the produced thermal medium. It is found that γs increases from about 0.5 to 1.0 in a narrow temperature range around the quark-hadron transition temperature Tc ≃ 160 MeV. Strangeness suppression thus disappears with the onset of color deconfinement; subsequently, full equilibrium resonance gas behavior is attained.

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